Optical disc and optical disc address reading apparatus and method

ABSTRACT

An optical disc having marks for dispersed addresses that can be easily detected with high precision. A dispersed address comprises synchronization marks, positive marks, and negative marks. Synchronization marks, positive marks, and negative marks are formed along a groove as partial discontinuities or partial modifications in the wobbled groove.

This is a divisional application of U.S. application Ser. No.10/615,799, filed Jul. 10, 2003, which is a divisional application ofU.S. application Ser. No. 10/169,915, filed Jul. 11, 2002, now U.S. Pat.No. 6,738,342 which is the National Stage of International ApnlicationNo. PCT/JP00/09347, filed Dec. 27, 2000.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to an optically rewritable optical discand to an apparatus and method for reading addresses prewritten to theoptical disc.

2. Description of Related Art

DVD-RAM, CD-RW, and MD are examples of user-recordable optical discsthat have become available in the last few years. This type ofrecordable optical disc has grooves formed along a spiral or pluralconcentric tracks with a phase change material or magneto-opticalmaterial formed on the groove surface. Addresses for specifying aparticular location on the disc are also pre-recorded to the tracksusing rewritable marks. This type of address is described in JapanesePatent Laid-Open Publication (kokai) H8-315426.

Kokai H8-315426 describes providing discontinuities in the grooves andusing these discontinuous parts for forming a pattern corresponding tothe address signal. A pattern corresponding to the address signal is abinary signal that inverts at each discontinuity, an on/off signal usedfor generating an ATIP (Absolute Time Pregroove) signal. Thediscontinuities are therefore used simply as a signal indicatingpresence or absence.

SUMMARY OF THE INVENTION

(Technical Problem to be Solved)

More address values and a method for more efficiently assigning addressvalues is needed in order to create an optical disc with an even higherrecording density. In an optical disc according to the related art,however, the discontinuities are nothing more than a trigger signal forsignal inversion and can carry only one piece of information (triggerdata). Numerous marks are therefore required.

Furthermore, the approximate location of a track can be detected withthe ATIP signal, but the position where recording starts cannot beprecisely determined. This means that when appending a new recordingafter recording once, or when overwriting data in the middle of aprevious recording, new data may be recorded over previously recordeddata that is still necessary. Crosstalk also occurs more easily when thetrack pitch is reduced.

The present invention is directed to a solution for these problems andprovides an optical disc wherein discontinuities or modifications are isformed in the grooves and two or more meanings are imparted to thediscontinuities or modifications in order to provide address informationmore efficiently.

A further object of the invention is to provide an optical disc wherebythe positioning precision of the recording start point can be increased.

A yet further object of the invention is to provide an optical discenabling the track pitch to be reduced.

A yet further object of the invention is to provide an optical disc thatis recordable and playable with full CLV (constant linear velocity)control.

A yet further object of the invention is to provide an apparatus andmethod of simple design for accurately reading address information froman optical disc having address information containing two or moremeanings imparted to discontinuities or modifications formed in thegrooves.

The invention as described in claim 1 is a rewritable optical disc witha spiral or concentric track comprising:

a groove formed with a sinusoidal wobble along the track;

a sector block disposed along the track;

sectors formed by dividing each sector block into a plurality of parts;

a synchronization mark formed in the first sector in each sector block;and

positive marks or negative marks formed in sectors other than the firstsector in each sector block;

-   -   each positive mark being a first groove discontinuity creating a        discontinuity of a first width W1 in the track direction of the        groove,    -   each negative mark being a second groove discontinuity creating        a discontinuity of a second width W0 in the track direction of        the groove, and    -   each synchronization mark being a third groove discontinuity        creating a discontinuity of a third width Ws in the track        direction.

The invention as described in claim 2 is an optical disc as described inclaim 1, wherein the first, second, and third groove discontinuitieshave a mirror surface.

The invention as described in claim 3 is an optical disc as described inclaim 1, wherein the first, second, and third groove discontinuities areformed in maximum amplitude parts of the wobble groove.

The invention as described in claim 4 is an optical disc as described inclaim 1, wherein the first, second, and third groove discontinuities areformed in the minimum amplitude part of the wobble groove.

The invention as described in claim 5 is an optical disc as described inclaim 1, wherein the first, second, and third widths W1, W0, and Ws areall longer than the longest mark contained in data recorded to a grooveand less than or equal to ½ wobble period.

The invention as described in claim 6 is an optical disc as described inclaim 1, wherein the first, second, and third widths W1, W0, and Ws areall longer than the longest mark contained in data recorded to a grooveand less than or equal to ¼ wobble period.

The invention as described in claim 7 is an optical disc as described inclaim 1, wherein the ratio between first, second, and third widths W1,W0, and Ws is 1:2:4 where any one of widths W1, W0, and Ws is 1.

The invention as described in claim 8 is an optical disc as described inclaim 1, wherein the ratio between first, second, and third widths W1,W0, and Ws is 2:1:4.

The invention as described in claim 9 is an optical disc as described inclaim 1, wherein the first, second, and third widths W1, W0, and Ws aretwo bytes, one byte, and four bytes, respectively.

The invention as described in claim 10 is a rewritable optical disc witha spiral or concentric track comprising:

a groove formed with a sinusoidal wobble along the track;

a sector block disposed along the track;

sectors formed by dividing each sector block into a plurality of parts;

a synchronization mark formed in the first sectorin each sector block;and

positive marks or negative marks formed in sectors other than the firstsector in each sector block;

each positive mark, negative mark, and synchronization mark being formedas a groove top offset portion where the groove is locally offset in afirst direction perpendicular to the track direction, a groove bottomoffset portion where the groove is locally offset in a second directionperpendicular to the track direction, or a combination of groove bottomoffset portions and groove top offset portions.

The invention as described in claim 11 is an optical disc as describedin claim 10, wherein:

a positive mark is a groove top offset portion;

a negative mark is a groove bottom offset portion; and

a synchronization mark is a combination of a groove top offset portionand groove bottom offset portion.

The invention as described in claim 12 is an optical disc as describedin claim 10, wherein the groove bottom offset portions and groove topoffset portions are disposed at maximum amplitude parts of the wobblegroove and are offset in a track center direction.

The invention as described in claim 13 is an optical disc as describedin claim 10, wherein groove bottom offset portions and groove top offsetportions of a synchronization mark are mutually adjacent at n+(½) wobblecycles (where n is a positive integer).

The invention as described in claim 14 is an optical disc as describedin claim 13, wherein n is 0.

The invention as described in claim 15 is a rewritable optical disc witha spiral or concentric track comprising:

a groove formed with a sinusoidal wobble along the track;

a sector block disposed along the track;

sectors formed by dividing each sector block into a plurality of parts;

a synchronization mark formed in the first sector in each sector block;and

positive marks or negative marks formed in sectors other than the firstsector in each sector block;

each positive mark, negative mark, and synchronization mark being formedby a groove ascending-phase inversion part for vertically phaseinverting an approximately ¼ wobble cycle part from a trough in thewobble groove, a groove descending-phase inversion part for verticallyphase inverting an approximately ¼ wobble cycle part from a peak in thewobble groove, or a combination of a groove ascending-phase inversionpart and groove descending-phase inversion part.

The invention as described in claim 16 is an optical disc as describedin claim 15, wherein a positive mark is formed by a grooveascending-phase inversion part, a negative mark is formed by a groovedescending-phase inversion part, and a synchronization mark is formed bya combination of a groove descending-phase inversion part and grooveascending-phase inversion part.

The invention as described in claim 17 is an optical disc as describedin claim 15, wherein both ends of said groove descending-phase inversionparts and groove ascending-phase inversion parts are a groovediscontinuity.

The invention as described in claim 18 is an optical disc as describedin claim 15, wherein both ends of said groove descending-phase inversionparts and groove ascending-phase inversion parts are an abruptlydisplaced groove.

The invention as described in claim 19 is a rewritable optical disc witha spiral or concentric track comprising:

a groove-formed with a sinusoidal wobble along the track;

a sector block disposed along the track;

sectors formed by dividing each sector block into a plurality of parts;

a synchronization mark formed in the first sector in each sector block;and

positive marks or negative marks formed in sectors other than the firstsector in each sector block;

each positive mark, negative mark, and synchronization mark being formedby a groove ascending-rectilinear portion connected to the wobble peakby forming the groove at a trough level from a trough in the wobblegroove to an approximately ¼ wobble cycle portion of the wobble groove,then abruptly changing to a peak level and forming the groove at thepeak level in the next ¼ wobble cycle portion,

-   -   a groove descending-rectilinear portion connected to the wobble        trough by forming the groove at a peak level from a peak in the        wobble groove to an approximately ¼ wobble cycle portion of the        wobble groove, then abruptly changing to a trough level and        forming the groove at the trough level in the next ¼ wobble        cycle portion, or    -   a combination of a groove descending-rectilinear portion and        groove ascending-rectilinear portion.

The invention as described in claim 20 is an optical disc as describedin claim 19, wherein a positive mark is formed by a grooveascending-rectilineare portion, a negative mark is formed by a groovedescending-rectilinear portion, and a synchronization mark is formed bya combination of a groove descending-rectilinear portion and grooveascending-rectilinear portion.

The invention as described in claim 21 is an optical disc as describedin claim 19, wherein each positive mark, negative mark, andsynchronization mark is formed by said groove ascending-rectilinearportion being repeated for a plurality of cycles of the wobbled groove,said groove descending-rectilinear portion being repeated for aplurality of cycles of the wobbled groove, or said combination of agroove descending-rectilinear portion and groove ascending-rectilinearportion being repeated for a plurality of cycles of the wobbled groove.

The invention as described in claim 22 is an optical disc as describedin claim 21, wherein each positive mark is formed by said grooveascending-rectilinear portion being repeated for a plurality of cyclesof the wobbled groove,

each negative mark is formed by said groove descending-rectilinearportion being repeated for a plurality of cycles of the wobbled groove,and

each synchronization mark is formed by said combination of a groovedescending-rectilinear portion and groove ascending-rectilinear portionbeing repeated for a plurality of cycles of the wobbled groove.

The invention as described in claim 23 is an address reading apparatusfor detecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 1 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

an optical head (2) for emitting a laser beam to a track of the opticaldisc and detecting reflected light by means of two photodetectorsseparated along the track direction;

a subtracter (4) for getting a difference of signals from the twophotodetectors and generating a difference signal;

a filter (6) for removing a wobble frequency component of a wobbledtrack and generating a groove discontinuity pulse;

a discriminator (12) for detecting a groove discontinuity pulse widthand discriminating each synchronization mark, positive mark, andnegative mark based on said width to generate a synchronization marksignal, positive mark signal, and negative mark signal; and

a demodulator (14) for generating 1s and 0s according to each positivemark signal and negative mark signal contained between onesynchronization mark signal and a next synchronization mark signal.

The invention as described in claim 24 is an address reading method fordetecting synchronization marks, positive marks, and negative to markscontained in an optical disc as described in claim 1 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

emitting a laser beam to a track of the optical disc and detectingreflected light by means of two photodetectors separated along the trackdirection;

getting a difference of signals from the two photodetectors andgenerating a difference signal;

removing a wobble frequency component of a wobbled track and generatinga groove discontinuity pulse;

detecting a groove discontinuity pulse width and discriminating eachsynchronization mark, positive mark, and negative mark based on saidwidth to generate a synchronization mark signal, positive mark signal,and negative mark signal; and

generating 1s and 0s according to each positive mark signal and negativemark signal contained between one synchronization mark signal and a nextsynchronization mark signal.

The invention as described in claim 25 is an address reading apparatusfor detecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 10 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

an optical head (2) for emitting a laser beam to a track of the opticaldisc and detecting reflected light by means of two photodetectorsseparated along the track direction;

a subtracter (4) for getting a difference of signals from the twophotodetectors and generating a difference signal;

a filter (6) for removing a wobble frequency component of a wobbledtrack and generating a groove bottom offset portion pulse in a negativedirection and a groove top offset portion pulse in a positive direction;

discriminators (52, 54, 12) for discriminating each synchronizationmark, positive mark, and negative mark based on said groove top offsetportion pulse, groove bottom offset portion pulse, and groove bottomoffset portion pulse and groove top offset portion pulse pair togenerate a positive mark signal, negative mark signal, andsynchronization mark signal; and

a demodulator (14) for generating 1s and 0s according to each positivemark signal and negative mark signal contained between onesynchronization mark signal and a next synchronization mark signal.

The invention as described in claim 26 is an address reading method fordetecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 10 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

emitting a laser beam to a track of the optical disc and detectingreflected light by means of two photodetectors separated along the trackdirection;

getting a difference of signals from the two photodetectors andgenerating a difference signal;

removing a wobble frequency component of a wobbled track and generatinga groove bottom offset portion pulse in a negative direction and agroove top offset portion pulse in a positive direction;

discriminating each synchronization mark, positive mark, and negativemark based on said groove top offset portion pulse, groove bottom offsetportion pulse, and groove bottom offset portion pulse and groove topoffset portion pulse pair to generate a positive mark signal, negativemark signal, and synchronization mark signal; and

generating 1s and 0s according to each positive mark signal and negativemark signal contained between one synchronization mark signal and a nextsynchronization mark signal.

The invention as described in claim 27 is an address reading apparatusfor detecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 15 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

an optical head (2) for emitting a laser beam to a track of the opticaldisc and detecting reflected light by means of two photodetectorsseparated along the track direction;

a subtracter (4) for getting a difference of signals from the twophotodetectors and generating a difference signal;

a filter (6) for removing a wobble frequency component of a wobbledtrack and generating a groove descending-phase inversion part pulse in anegative direction and a groove ascending-phase inversion part pulse ina positive direction;

discriminators (52, 54, 12) for discriminating each synchronizationmark, positive mark, and negative mark based on said grooveascending-phase inversion part pulse, groove descending-phase inversionpart pulse, and groove descending-phase inversion part pulse and grooveascending-phase inversion part pulse pair to generate a positive marksignal, negative mark signal, and synchronization mark signal; and

a demodulator (14) for generating 1s and 0s according to each positivemark signal and negative mark signal contained between onesynchronization mark signal and a next synchronization mark signal.

The invention as described in claim 28 is an address reading method fordetecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 15 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

emitting a laser beam to a track of the optical disc and detectingreflected light by means of two photodetectors separated along the trackdirection;

getting a difference of signals from the two photodetectors andgenerating a difference signal;

removing a wobble frequency component of a wobbled track and generatinga groove descending-phase inversion part pulse in a negative directionand a groove ascending-phase inversion part pulse in a positivedirection;

discriminating each synchronization mark, positive mark, and negativemark based on said groove ascending-phase inversion part pulse, groovedescending-phase inversion part pulse, and groove descending-phaseinversion part pulse and groove ascending-phase inversion part pulsepair to generate a positive mark signal, negative mark signal, andsynchronization mark signal; and

generating 1s and 0s according to each positive mark signal and negativemark signal contained between one synchronization mark signal and a nextsynchronization mark signal.

The invention as described in claim 29 is an address reading apparatusfor detecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 19 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

an optical head (2) for emitting a laser beam to a track of the opticaldisc and detecting reflected light by means of two photodetectorsseparated along the track direction;

a subtracter (4) for getting a difference of signals from the two isphotodetectors and generating a difference signal;

a filter (6) for removing a wobble frequency component of a wobbledtrack and generating a groove descending-rectilinear portion pulse in anegative direction and a groove ascending-rectilinear portion pulse in apositive direction;

discriminators (52, 54, 12) for discriminating each synchronizationmark, positive mark, and negative mark based on said grooveascending-rectilinear portion pulse, groove descending-rectilinearportion pulse, and groove descending-rectilinear portion pulse andgroove ascending-rectilinear portion pulse pair to generate a positivemark signal, negative mark signal, and synchronization mark signal; and

a demodulator (14) for generating 1s and 0s according to each positivemark signal and negative mark signal contained between onesynchronization mark signal and a next synchronization mark signal.

The invention as described in claim 30 is an address reading method fordetecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 19 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

emitting a laser beam to a track of the optical disc and detectingreflected light by means of two photodetectors separated along the trackdirection;

getting a difference of signals from the two photodetectors andgenerating a difference signal;

removing a wobble frequency component of a wobbled track and generatinga groove descending-rectilinear portion pulse in a negative directionand a groove ascending-rectilinear portion pulse in a positivedirection;

discriminating each synchronization mark, positive mark, and negativemark based on said groove ascending-rectilinear portion pulse, groovedescending-rectilinear portion pulse, and groove descending-rectilinearportion pulse and groove ascending-rectilinear portion pulse pair togenerate a positive mark signal, negative, mark signal, andsynchronization mark signal; and

generating 1s and 0s according to each positive mark signal and negativemark signal contained between one synchronization mark signal and a nextsynchronization mark signal.

The invention as described in claim 31 is an address reading apparatusfor detecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 21 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

an optical head (2) for emitting a laser beam to a track of the opticaldisc and detecting reflected light by means of two photodetectorsseparated along the track direction;

a subtracter (4) for getting a difference of signals from the twophotodetectors and generating a difference signal;

a filter (6) for removing a wobble frequency component of a wobbledtrack and generating a groove descending-rectilinear portion pulse in anegative direction and a groove ascending-rectilinear portion pulse in apositive direction;

a first counter (93) for counting a number of groovedescending-rectilinear portion pulses in a negative direction containedin one sector;

a second counter (94) for counting a number of grooveascending-rectilinear portion pulses in a positive direction containedin one sector;

discriminators (95 to 99) for comparing a first count from the firstcounter and a second count from the second counter and discriminatingeach synchronization mark, positive mark, and negative mark according towhether the first count is sufficiently high, the second count issufficiently high, or the first count and second count are substantiallyequal to generate a positive mark signal, negative mark signal, andsynchronization mark signal; and

a demodulator (14) for generating 1s and 0s according to each positivemark signal and negative mark signal contained between onesynchronization mark signal and a next synchronization mark signal.

The invention as described in claim 32 is an address reading method fordetecting synchronization marks, positive marks, and negative markscontained in an optical disc as described in claim 21 and accumulating 1and 0 data obtained from positive marks and negative marks dispersedlycontained in one sector block to read said sector block address,comprising:

emitting a laser beam to a track of the optical disc and detectingreflected light by means of two photodetectors separated along the trackdirection;

getting a difference of signals from the two photodetectors andgenerating a difference signal;

removing a wobble frequency component of a wobbled track and generatinga groove descending-rectilinear portion pulse in a negative directionand a groove ascending-rectilinear portion pulse in a positivedirection;

counting a number of groove descending-rectilinear portion pulses in anegative direction contained in one sector as a first count;

counting a number of groove ascending-rectilinear portion pulses in apositive direction contained in one sector as a second count;

comparing the first count and second count and discriminating eachsynchronization mark, positive mark, and negative mark according towhether the first count is sufficiently high, the second count issufficiently high, or the first count and second count are substantiallyequal to generate a positive mark signal, negative mark signal, andsynchronization mark signal; and

generating 1s and 0s according to each positive mark signal and negativemark signal contained between one synchronization mark signal and a nextsynchronization mark signal.

The invention as described in claim 33 is an optical disc as describedin claim 19, wherein the synchronization mark further has a block markindicating a sector block starting position.

The invention as described in claim 34 is an optical disc as describedin claim 33, wherein said block mark is formed by disposing adiscontinuity in the track groove.

The invention as described in claim 35 is an optical disc as describedin claim 33, wherein said block mark is formed by locally changing awidth of the track groove.

The invention as described in claim 36 is an optical disc as describedin claim 33, wherein said block mark is formed by locally changingwobble amplitude.

The invention as described in claim 37 is an optical disc as describedin claim 19, wherein each wobble cycle is formed so that the duty ratiodiffers according to positive data and negative data.

The invention as described in claim 38 is an optical disc as describedin claim 19, wherein only one edge of the track groove is wobbled.

(Advantages Over the Related Art)

Meaning other than simply identifying the presence or absence of amodification can be imparted to each groove modification by forminggroove modifications of multiple different shapes in a wobble groove.More information can therefore be recorded with fewer groovemodifications.

An address reader of simple configuration according to the presentinvention can also accurately and efficiently read dispersed addresses.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1A is a plan view of an optical disc according to a preferredembodiment of the present invention, and FIG. 1B is a schematic view ofa sector block;

FIG. 2A is descriptive drawing of a dispersed address recorded to thecenter block, and FIG. 2B is a schematic drawing of a groove in whichdispersed address marks are formed;

FIG. 3 is a partially enlarged view of an optical disc having groovediscontinuities according to a preferred embodiment of the invention;

FIG. 4 is a block diagram of an address reader for an optical disc asshown in FIG. 3;

FIG. 5 is a waveform diagram of signals at essential points in theaddress reader shown in FIG. 4;

FIG. 6 is a block diagram of the discriminator shown in FIG. 4;

FIG. 7 is a block diagram of the demodulator shown in FIG. 4;

FIG. 8 is an enlarged view showing the groove offset part as a tofurther example of a groove discontinuity;

FIG. 9 is an enlarged view showing the groove offset part as a furtherexample of a groove discontinuity;

FIG. 10 is a partial enlarged view of an optical disc having marksformed by the groove offset parts according to a second embodiment ofthe invention;

FIG. 11 is a block diagram of an address reader for the optical discshown in FIG. 10;

FIG. 12 is a waveform diagram of the output signal from the subtractershown in FIG. 11 using the optical disc shown in FIG. 10;

FIG. 13 is a waveform diagram of the output signal from the filter shownin FIG. 11 using the optical disc shown in FIG. 10;

FIG. 14 is a waveform diagram of the output signal from the comparatorshown in FIG. 11 using the optical disc shown in FIG. 10;

FIG. 15 is an enlarged view of a discontinuous groove phase inversionpart;

FIG. 16 is an enlarged view of a continuous groove phase inversion part;

FIG. 17 is a partial enlarged view of an optical disc having marksresulting from the groove phase inversion parts;

FIG. 18 is a waveform diagram of the output signal from the subtractershown in FIG. 11 using the optical disc shown in FIG. 17;

FIG. 19 is a waveform diagram of the output signal from the filter shownin FIG. 11 using the optical disc shown in FIG. 17;

FIG. 20 is a waveform diagram of the output signal from the comparatorshown in FIG. 11 using the optical disc shown in FIG. 17;

FIG. 21 is an enlarged view of the rectilinear portion of the groove;

FIG. 22 is a partial enlarged view of an optical disc having marksformed by a rectilinear portion of the groove;

FIG. 23 is a waveform diagram of the output signal from the subtractershown in FIG. 11 using the optical disc shown in FIG. 22;

FIG. 24 is a waveform diagram of the output signal from the filter shownin FIG. 11 using the optical disc shown in FIG. 22;

FIG. 25 is a waveform diagram of the output signal from the comparatorshown in FIG. 11 using the optical disc shown in FIG. 22;

FIG. 26 is an enlarged view of an optical disc having groovediscontinuities unifying the recording start positions;

FIG. 27 is an enlarged view of an optical disc having marks formed byconsecutive rectilinear groove portions;

FIG. 28 is a waveform diagram of the output signal from the subtracterof the rectilinear wave detector in FIG. 31 using an optical disc asshown in FIG. 27;

FIG. 29 is a waveform diagram of the output signal from the filter ofthe rectilinear wave detector in FIG. 31 using an optical disc as shownin FIG. 27;

FIG. 30 is a waveform diagram of the output signal from the comparatorof the rectilinear wave detector in FIG. 31 using an optical disc asshown in FIG. 22;

FIG. 31 is a block diagram of an address reader for an optical disc asshown in FIG. 27;

FIG. 32 is a plan view of a wobble in which the duty ratio varies;

FIG. 33 is a plan view of a block mark;

FIG. 34 is a plan view of another block mark; and

FIG. 35 is an oblique view showing the wobble disposed to only one sideof the groove.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The preferred embodiments of the present invention are described belowwith reference to the accompanying figures.

Embodiment 1

FIG. 1A is a plan view of an optical disc according to a preferredembodiment of the present invention, and FIG. 1B describes the placementof sector blocks. Shown in FIG. 1A are the optical disc substrate 101,header 102 that is preformed when the disc is made, recording area 103where data can be recorded, and sector 104, which is the data recordingunit. FIG. 1B shows a sector block 105 containing a specific number(such as 32) of sectors.

A phase change film is formed on the optical disc substrate 101. Data isrecorded to this phase change film by optically changing this phasechange film between amorphous and crystalline phases, and signals areread using the difference in reflectivity between amorphous and crystalphase parts.

The relationship between sectors 104 and sector block 105 is describedin detail next with reference to FIG. 2A.

In an optical disc according to this embodiment of the invention a trackcomprises a number of consecutive sector blocks 105. As noted above,each sector block 105 contains 32 sectors 104. Each sector 104 startswith a header 102 followed by a recording area 103 where signals arerecorded and reproduced. A sector is 2448 bytes long.

A synchronization mark S is recorded in the header 102 of the firstsector 104 in each sector block 105. The start of a sector block 105 canbe detected by detecting this synchronization mark S.

A positive mark or negative mark is recorded in the header 102 of thesecond sector 104 in each sector block 105. A value of 1 is belowassumed to be assigned to positive marks and a value of 0 assigned tonegative marks. In the example shown in FIG. 2A, a negative mark 0 isrecorded to the header 102 of the second sector 104. It is thus possibleto assign one bit of information to the header in the second andsuccessive sectors 104 (referred to below as successive sectors).

It is therefore possible to generate 31 bits of information using thesynchronization mark S and the following positive marks (1) and negativemarks (0) by accumulating these data bits from the headers of the 32sectors in a sector block 105. Stated another way, 31 bits ofinformation can be dispersed one bit at a time to the 31 sectors 104 ina sector block 105, and a synchronization mark is disposed at thebeginning of each sector block 105 so that the start of each sectorblock 105 can be detected. An address having 0 and 1 bits thus dispersedis referred to herein as a “dispersed address.”

These 31 bits include 19 bits of primary data and 12 bits of secondarydata. The 19-bit primary data identifies the sector block 105 position.This enables detecting the location of (2 to the 19th power=) 524,288sector blocks 105. This means that if the address of the first sectorblock in the optical disc is 0 and the sector block address valueincrements 1 at each successive sector block, the value yielded by the19-bit primary data is the absolute address of each sector block 105,and each sector 104 stores 2048 bytes of data and each sector block 105thus stores 65,536=(2048*32) bytes, then addresses enabling a maximum 34gigabytes of data can be assigned using this 19-bit address data.

The 12-bit secondary data is allocated to an error correction codeenabling correction if any particular bit in the 19-bit primary data or12-bit secondary data is dropped because of a disc defect, for example,or is erroneously detected during playback. This could be an errorcorrection code for all 31 data bits. Furthermore, because the sectorblock 105 address value increments one in each successive sector block105 and the higher bits can be predicted from a preceding sector block105, the 12-bit secondary data could be an error correction code for thelower 8-bits.

A dispersed address, is described in further detail in Japanese PatentApplication H11-343060.

As shown in FIG. 2B, an optical disc 101 according to the presentinvention has multiple spiral or concentric (spiral in this embodiment)tracks divided into sectors. In the example shown in FIG. 1A sectorheaders (containing the synchronization mark S, positive mark (1) ornegative mark (0)) are aligned along virtual lines in the radialdirection of the disc, but the headers do not align in any radialdirection in the example shown in FIG. 2B.

As shown in FIG. 3, the tracks are grooves and the space betweenadjacent tracks, such as the space between groove n and groove n+1, is aland. The lands have a mirror surface. The grooves are wave-shapedwobble grooves. The wobble wave has a frequency of 153 cycles persector, for example. The wobble period thus corresponds to 16 bytes. Ifthe data is recorded with 8–16 modulation and one clock period is T, theshortest mark is 3T and the longest mark is 14T, and one byte is 16T.

In this embodiment of the invention a positive mark (1) is formed by adiscontinuity of width W1 in the track direction in the first groove, anegative mark (0) is formed by a discontinuity of a width 0 in the trackdirection in a second groove, and a synchronization mark S is formed bya discontinuity of width Ws in the track direction in a third groove.These groove discontinuities have a mirror surface such as found in thelands.

The synchronization marks S, positive marks, and negative marks do notneed to be aligned in the radial direction of the optical disc. Thesector length can therefore be the same at any position on the disc, andfull CLV control can be achieved.

Recording start positions can also be precisely determined becauserecording can start immediately following a groove discontinuity.

Synchronization marks, positive marks, and negative marks can be formedusing the groove discontinuities as follows.

Before the grooves are formed the optical disc has a mirror surfacecoated with a photoresist. The wobble grooves are formed by emitting alaser oscillating perpendicularly to the track while the disc rotates.When the laser is interrupted during groove formation a discontinuityresulting in a synchronization mark S, positive mark (1), or negativemark (0) is formed in the groove with the length of the discontinuitydetermined by how long laser emission is interrupted. In a preferredembodiment of the invention the synchronization marks S, positive marks(1), and negative marks (0) are formed at the peaks or troughs of thewobble groove, that is, where the amplitude is greatest, in order tomake the groove discontinuities easier to detect. A single beam lasercan therefore be used to cut the grooves by thus forming the marks ingroove discontinuities.

The widths Ws, W1, W0 of the groove discontinuities corresponding tosynchronization mark S, positive mark (1), and negative mark (0),respectively, are determined as follows.

Mark width is preferably greater than the longest mark in the recordeddata (i.e., longer than 14T in the present example) so that recordeddata signals that leak into the tracking error signal as noise are notmistakenly recognized as a dispersed address, that is, a signal from asynchronization mark S, positive mark (1), or negative mark (0).

Furthermore, the synchronization marks S, positive marks (1), andnegative marks (0) are disposed where wobble signal amplitude isgreatest. Mark width must therefore be less than ½ the wobble period andpreferably ¼ or less of the wobble period in order to improve detectionprecision.

The width W of the groove discontinuity corresponding to anysynchronization mark S, positive mark (1), or negative mark (0) istherefore14T<W<(wobble period/2)  (1)and preferably14T<W<(wobble period/4).  (2)To satisfy these conditions (1) and (2) and enable the widths of thegroove discontinuities denoting a synchronization mark S, positive mark(1), or negative mark (0) to be easily identified, the width ratio ofthese marks is set to 4:2:1, for example. While the ratio of the groovediscontinuities could be 4:4:4, groove discontinuities in the thirdgroove corresponding to the marks that are most important to recognize,i.e., synchronization marks S, are preferably 4, discontinuitiescorresponding to the positive marks (1) are 2 (or 1), anddiscontinuities corresponding to the negative marks (0) are 1 (or 2).Yet more specifically, the widths of these groove discontinuities are asfollow.

-   third groove discontinuities (synchronization marks S)=4 bytes

first groove discontinuities (positive marks (1))=2 bytes

second groove discontinuities (negative marks (0))=1 byte

It will be noted that in addition to expressing whether or not a groovediscontinuity is present, these groove discontinuities also expressthree different meanings (that is, positive mark (1), negative mark (0),and synchronization mark S) depending upon the length of the groovediscontinuity.

FIG. 4 shows a device for reading dispersed addresses such as shown inFIG. 3, and FIG. 5 is a waveform diagram of output signals at importantpoints in the address reader. Referring to FIG. 4, this address readerhas an optical head 2, subtracter 4, high pass filter 6, comparator 8,discriminator 12, and demodulator 14. The optical head 2 has alight-emitting element 2 c for emitting a laser beam, and photodetectors2 a, 2 b offset from each other across the track center. The subtracter4 obtains the difference of the signals output from photodetectors 2 a,2 b, and outputs difference signal Sa (FIG. 5). The high pass filter 6passes high frequency components and outputs groove discontinuity signalSb (FIG. 5). The comparator 8 compares the groove discontinuity signalSb with a specific threshold value Sc supplied from threshold valuecontroller 10 and outputs a binary groove discontinuity signal Sd (FIG.5). The discriminator 12 then determines if the digitized groovediscontinuity signal Sd corresponds to a first groove discontinuity(positive mark (1)), second groove discontinuity (negative mark (0)) orthird groove discontinuity (synchronization mark S). The demodulator 14accumulates the 31 positive marks (1) and negative marks (0) followingeach synchronization mark S to assemble the dispersed address valuesinto a single continuous address value. The difference signal Sa outputfrom the subtracter 4 is a push-pull signal, and can therefore be usedas a tracking error signal.

As shown in FIG. 5 the difference signal Sa describes a sinusoidal wavecorresponding to the track wobble. The difference signal Sa drops tozero wherever a groove discontinuity exists, and the signal leveltherefore drops to zero for a pulse width determined by the width of thediscontinuity. The low frequency wave component (the wobble sine wave)is removed from the groove discontinuity signal Sb output by comparator8, which acts as a filter, and groove discontinuity signal Sb thereforecontains only pulses from the groove discontinuities. These pulses arecompared with a specific threshold value to generate the digital groovediscontinuity signal Sd.

FIG. 6 shows the discriminator 12 in detail. The pulse width detector 22of this discriminator 12 receives the digital groove discontinuitysignal Sd and detects the pulse width therefrom. If the detected pulsewidth of the groove discontinuity signal Sd is 14T or less, the signalis passed to ignore processor 24 and ignored.

If the detected pulse width of the groove discontinuity signal Sd is 14Tor greater and 24T or less, the signal is passed to output-0 processor26, which thus recognizes a second groove discontinuity signal andoutputs signal Se denoting a 0 (FIG. 5). This signal Se is reset by thenext groove discontinuity signal Sd.

If the detected pulse width of the groove discontinuity signal Sd is 24Tor greater and 48T or less, the signal is passed to output-1 processor28, which thus recognizes a first groove discontinuity signal andoutputs signal Sf denoting a 1 (FIG. 5). This signal Sf is reset by thenext groove discontinuity signal Sd.

If the detected pulse width of the groove discontinuity signal Sd is 48Tor greater and 80T or less, the signal is passed to output-S processor30, which thus recognizes a third groove discontinuity signal andoutputs signal S denoting the beginning of a sector block. This signal Sis reset by the next groove discontinuity signal Sd.

If the pulse width of the detected groove discontinuity signal Sd is 80Tor greater, the signal is passed to ignore processor 32 and ignored. Itwill be obvious that signal Se denoting a 0 corresponds to a negativemark (0), signal Sf denoting a 1 corresponds to a positive mark (1), andsignal S corresponds to a synchronization mark S.

Signal Se denoting a 0 output from output-0 processor 26, signal Sfdenoting a 1 output from the output-1 processor 28, and signal S fromthe output-S processor 30 are output to the demodulator 14, whichrecognizes the dispersed address as a single address.

It will thus be clear that in addition to detecting whether or not thegroove is present, the discriminator 12 generates signals with threedifferent meanings (that is, signal Sf denoting 1, signal Se denoting 0,and signal S denoting a synchronization mark) based on the length of thegroove discontinuity signal.

FIG. 7 shows the configuration of demodulator 14 in detail. An encoder42 converts signal Se to a 1-bit 0 signal and signal Sf to a 1-bit 1signal. The encoder 42 outputs to the shift register 44, which convertsthe 1-bit 0 and 1 signals of the 31-bit serial dispersed address to aparallel address. The latch 46 latches the 31-bit address signal in theshift register 44 at signal S. A parity coder 48 uses the low 12 bits ofthe 31 address bits for a parity check code. The error correctionprocessor 50 uses this parity check code for error correction of thehigh 19 address bits of the 31 address bits. The demodulator 14 thusoutputs a 19-bit address for each sector block.

It should be noted that depending on the type of optical disc thegrooves may refer to trenches or to the lands between trenches. Notethat data can later be written to the mirror surface header 102.

The address reader described above features a simple configuration ableto efficiently read dispersed addresses. It will also be noted that thesynchronization marks, positive marks, and negative marks are read usinga difference signal and can therefore be easily separated from datasignals recorded to the grooves.

Furthermore, forming the synchronization marks, positive marks, andnegative marks within the width of the maximum wobble amplitude preventsan increase in crosstalk between adjacent tracks.

Full CLV control from inside to outside disc circumference can also beachieved because the sectors are formed without changing the sectorlength between the inside and outside circumference and it is notnecessary to align sector block boundaries in the radial direction ofthe disc. When the boundaries between the sectors and sector blockswhere headers are written are aligned in adjacent tracks concentrated inthe radial direction of the disc as they are in a zone CLV disc as shownin FIG. 1A, the optical transmittance of the optical disc recordinglayer differs greatly between the header areas and non-header areas.Different transmittance values create no problem when the optical dischas only one recording layer. When the optical disc has two or morerecording layers, however, local variations in recording layertransmittance produce crosstalk between top and bottom layers, anddifferent transmittance values are therefore undesirable. An opticaldisc according to the present invention as shown in FIG. 2B, however,enables full CLV control, does not require that the headers besubstantially aligned in the radial direction of the disc; the headerscan therefore be dispersed, and interlayer crosstalk can be reduced in amultilayer optical disc.

Disc capacity can also be increased using full CLV control compared withzone CLV because unused space can be reduced.

The grooves, synchronization marks, positive marks, and negative markscan also be cut using a single beam.

Furthermore, groove discontinuities are formed in the optical discdescribed above by interrupting the laser beam used to cut the grooves,but can alternatively be formed as shown in FIG. 8 and FIG. 9 bymomentarily shifting the laser beam to form groove offset part 62 or 63.The offset time of the laser is adjusted to control the resultingdiscontinuities.

It should be noted that the identification marks are disposed at thebeginning of each sector in the present embodiment but shall not belimited thereto. The marks could, for example, be detected at the end ofthe sector.

An optical disc according to the first embodiment described above hasgroove discontinuities of different lengths formed in the header 102 atthe beginning of each sector with each groove discontinuity meaning asynchronization mark S, positive mark (1), or negative mark (0), therebyenabling sector block addresses to be encoded in less space.

Furthermore, an optical disc according to the present invention issuitable as a high density optical disc that is readable and recordableusing an approximately 400 nm wavelength laser from the light-emittingelement 2 c. The reasons for this are described below.

An optical disc according to the present invention is a recordable,readable optical disc having a crystal phase (unrecorded state)phase-change material formed on the disc surface in the grooves. Thisphase change material is, for example, a germanium-antimony compound ora silver-indium compound. Data is recorded by emitting a laser beam at aspecific recording power level to this phase change material to changethe crystal phase (unrecorded state) to amorphous phase (recorded state)marks. Reflectivity is different in the crystal phase and amorphousphase parts of the groove. Data can therefore be read by emitting alaser beam at a lower power level, and detecting differences inreflected light from the crystal phase and amorphous phase parts of thegroove to reproduce the recorded data. If the laser beam is in the 830nm or 650 nm waveband, reflections from the amorphous phase (recordedstate) parts will be weaker than reflections from the crystal phase(unrecorded state) parts. Furthermore, reflections from the mirror areasare stronger than reflections from the crystal phase parts. Reflectionsfrom the mirror, crystal phase, and amorphous phase parts can thus beranked as strong, medium, and weak, and the three parts can be easilyidentified.

If a 400 nm laser is used, however, the order of reflectivity changes:reflection from amorphous phase (recorded state) parts is stronger thanreflections from crystal phase (unrecorded state) parts. Reflectionsfrom the mirror, crystal phase, and amorphous phase parts are thereforeranked slightly strong, medium, strong, and identifying mirror partsfrom amorphous phase (recorded) parts becomes difficult. With an opticaldisc according to the present invention, however, the width of themirror-surface groove discontinuities is distinctly different from thewidth of the recording marks, and the groove discontinuities cantherefore be easily distinguished from the recording marks.

Embodiment 2

In an optical disc according to this second embodiment of the inventiondispersed addresses are recorded using groove modifications, morespecifically using a groove bottom offset 65, a groove top offset 66,and a combination 67 of groove bottom offset 65 and groove top offset 66as shown in FIG. 10. In the example shown in FIG. 10 a single groove topoffset 66 denotes a positive mark (1); a combination 67 containing agroove bottom offset 65 and a groove top offset 66 appearing within aspecified time of the groove bottom offset 65 denotes a synchronizationmark S; and a groove bottom offset 65 not followed by a groove topoffset 66 within a specific time denotes a negative mark (0). The groovebottom offsets and groove top offsets are generically referred to hereinas simply “groove offsets.” Any one of these parts 65, 66, 67 can beused as a synchronization mark, positive mark, or negative mark, butcombination 67 is preferably used as the synchronization marks, whichare detected less frequently. The same applies to the alternativeversions of this embodiment described below.

A groove bottom offset 65 is formed by creating a momentary offsettoward the track center from a peak in the wobble groove. A groove topoffset 66 is formed by creating a momentary offset toward the trackcenter from the bottom of a trough in the wobble groove. A combination67 is formed by creating a groove bottom offset 65 in a peak and agroove top offset 66 in the adjacent trough of the wobble groove.

Note that the groove bottom offset 65 and groove top offset 66 in acombination 67 shown in FIG. 10 are separated ½ wobble period, but couldbe separated (n+½) (where n is a positive integer) wobble period. Note,further, that the groove bottom offset could be formed as shown in FIG.9 instead of as in FIG. 8. The groove top offsets could also be formedin the same manner.

FIG. 11 shows an address reader for reading dispersed addresses encodedas shown in FIG. 10, and FIGS. 12 to 14 are waveform diagrams of theoutput signals at major points in the address reader. Like parts in theaddress reader shown in FIG. 4 and the address reader in FIG. 11 areidentified by like reference numerals and further description thereof isomitted below. Shown in FIG. 11 are optical head 2, subtracter 4outputting difference signal Sa (FIG. 12), high pass filter 6 foroutputting groove discontinuity (offset) signal Sb (FIG. 13),comparators 52 and 54, discriminator 56, and demodulator 14. Comparator52 compares groove discontinuity (top offset) signal Sb with specificfirst threshold value +Vth (FIG. 13) to output digital groove top offsetsignal Si (FIG. 14). Comparator 54 compares groove discontinuity (bottomoffset) signal Sb with specific second threshold value −Vth (FIG. 13) tooutput digital groove bottom offset signal Sj (FIG. 14). Discriminator56 detects whether the digitized groove top/bottom offset signals Si andSj correspond to a first groove offset (positive mark (1)), secondgroove offset (negative mark (0)), or third groove offset(synchronization mark S). Demodulator 14 compiles the dispersed addressinto a single continuous address value.

Signal Sa (S) in FIG. 12 is the difference signal for both groove bottomoffset 65 and groove top offset 66 in combination 67; signal Sa(0) isthe difference signal for groove bottom offset 65 only; and signal Sa(1)is the difference signal for groove top offset 66 only. A negative pulseis produced when there is a downward offset at a peak of the wobblegroove, and a positive pulse is generated when there is an upward offsetin a trough of the wobble groove.

Waveforms for signals Sa(S), Sa(0), and Sa(1) after removing lowfrequency components are shown as signals Sb(S), Sb(0), and Sb(1) inFIG. 13.

Signals Si(S), Sj(S) in FIG. 14 show the digital pulse signals derivedfrom the positive and negative pulses in signals Sb(S), Sb(0), and Sb(1)shown in FIG. 13. Because signal Sb(S) contains both positive andnegative pulses, a pulse is present in both signals Si(S) and Sj(S).Because signal Sb(0) contains only a negative pulse, however, a pulse ispresent in signal Sj(0) but not in Si(0). Likewise, because signal Sb(1)only has a positive pulse, a pulse is present in Si(1) but not in Sj(1).

The discriminator 56 operates as follows.

If either pulse signal Si or Sj is received and the other pulse signal(Si or Sj) is then also received within a specific period of time(within ½ wobble period), synchronization mark S is detected and signalS indicating the synchronization mark S is therefore output. Thissynchronization signal S is held until the next mark is detected.

If pulse signal Sj is not received within a specific time (within ½wobble period) after pulse signal Si is received, positive mark (1) isdetected and a “1” signal is output indicating the positive mark (1).This “1” signal is held until the next mark is detected.

If pulse signal Si is not received within a specific time (within ½wobble period) after pulse signal Sj is received, negative mark (0) isdetected and a “0” signal is output indicating the negative mark (0).This “0” signal is held until the next mark is detected.

Signals S, 1, and 0 are signals as shown in the bottom two rows of FIG.5, and are output from the three output lines of the discriminator 56shown in FIG. 11.

The demodulator 14 thereafter operates in the same way as thedemodulator shown in FIG. 7.

In addition to indicating whether there is an offset, the groove bottomoffset 65 and groove top offset 66 contain information indicating thedirection of the offset. Separate signals Si and Sj can therefore begenerated.

Groove bottom offset 65 and groove top offset 66 can also be used toidentify three different meanings (S, 0, 1) in ½ wobble period.

Crosstalk between adjacent tracks also does not occur because thesynchronization marks, positive marks, and negative marks are within thewidth of a maximum amplitude part of the wobble.

Full CLV control is also possible because the sectors are configuredwithout changing the sector length from the inside circumference to theoutside circumference of the optical disc and it is not necessary toalign the sector block borders in the radial direction of the disc.

The grooves, synchronization marks, positive marks, and negative markscan also be cut using a single laser beam.

Yet further, because the synchronization marks, positive marks, andnegative marks are formed offset from the track center, intermixing ofdata signals with the synchronization mark, positive mark, and negativemark detection signals is minimal even when data is recorded along thetrack center.

It is also possible to reliably detect groove offsets when the grooveoffsets are detected with a push-pull signal because the differencesignal is large.

First Alternative Embodiment

A first alternative version of the groove modifications in the secondembodiment of the invention is described below with reference to FIG. 15to FIG. 20.

While groove bottom offset 65 and groove top offset 66 are used in theembodiment shown in FIG. 10, these are changed to groovedescending-phase inversion part 74 and groove ascending-phase inversionpart 75 in this first alternative embodiment as shown in FIG. 17. Thegroove descending-phase inversion part 74 vertically inverts the phaseof the sinusoidal wobble wave from the groove peak to the groove trough,that is, an approximately ¼ phase segment of the wobble period from thegroove peak. The groove ascending-phase inversion part 75 similarlyvertically inverts the phase of the sinusoidal wobble wave from thegroove trough to the groove peak, that is, an approximately ¼ phasesegment of the wobble period from the groove trough. The groovedescending-phase inversion and groove ascending-phase inversion partsare together referred to as the groove phase inversion parts.

As shown in FIG. 17, a synchronization mark S is expressed by acombination 76 of consecutive groove descending-phase inversion 74 andgroove ascending-phase inversion 75 parts. A negative mark (0) containsonly groove descending-phase inversion part 74, and a positive mark (1)contains only groove ascending-phase inversion part 75. The ends of the¼ wobble period segments can be discontinuities in the groove asindicated in FIG. 16 or sudden displacements in the groove as shown inFIG. 16.

These marks can be read with an address reader as shown in FIG. 11.

FIG. 18 shows the difference signals for the groove phase inversionscorresponding to the three marks shown in FIG. 17. These differencesignals are output from the subtracter 4. As will be known fromdifference signal Sa(S), a difference signal that drops abruptly to theright is obtained where the phase inverts and there is an abrupttop-to-bottom change in the groove, and a difference signal that risesabruptly to the right is obtained where the phase inverts and there isan abrupt bottom-to-top change in the groove.

FIG. 19 shows the difference signal after it passes the high pass filter6. A difference signal that drops abruptly to the right appears as anegative pulse, and a difference signal that rises abruptly to the rightappears as a positive pulse.

FIG. 20 shows signal Si as the digitized version of the positive pulseoutput by comparator 52, and signal Sj as the digitized version of thenegative pulse output by comparator 54.

Discriminator 56 operates as follows in this case.

If either pulse signal Si or Sj is received and the other pulse signal(Si or Sj) is then also received within a first specific period of time(within the wobble period), synchronization mark S is detected andsignal S indicating the synchronization mark S is therefore output. Thissynchronization signal S is held until the next mark is detected.

If a second pulse signal Si is received within a second specific time(within ½ wobble period) after a first pulse signal Si is received,positive mark (1) is detected and a “1” signal is output indicating thepositive mark (1). The further condition that pulse signal Sj is notdetected between the first and second pulse signals Si can also beapplied. This “1” signal is held until the next mark is detected.

If a second pulse signal Sj is received within a second specific time(within ½ wobble period) after a first pulse signal Sj is received,negative mark (0) is detected and a “1” signal is output indicating thenegative mark (0). The further condition that pulse signal Si is notdetected between the first and second pulse signals Sj can also beapplied. This “0” signal is held until the next mark is detected.

Subsequent signal processing is handled by the demodulator 14 asdescribed above.

In addition to indicating whether there is a phase inversion, the groovedescending-phase inversion 74 and groove ascending-phase inversion 75parts contain information indicating the inversion direction. Separatesignals Si and Sj can therefore be generated.

Groove descending-phase inversion part 74 and groove ascending-phaseinversion part 75 can also be used to identify three different meanings(S, 0, 1) in one wobble period.

Crosstalk between adjacent tracks also does not occur because thesynchronization marks, positive marks, and negative marks are within thewidth of the maximum amplitude part of the wobble.

Full CLV control is also possible because the sectors are configuredwithout changing the sector length from the inside circumference to theoutside circumference of the optical disc and it is not necessary toalign the sector block borders in the radial direction of the disc.

The grooves, synchronization marks, positive marks, and negative markscan also be-cut using a single laser beam.

Furthermore, because the phase inverts where wobble amplitude isgreatest, the locations of the synchronization mark S, positive mark(1), or negative mark (0) can be detected with good precision.

It should be noted that the groove descending-phase inversion part 74and groove ascending-phase inversion part 75 could also be detected bydetecting the wobble phase. This results in a greater improvement in theS/N ratio than does detecting the phase inversion edge.

Second Alternative Embodiment

A second alternative version of the groove modifications in the secondembodiment of the invention is described below with reference to FIG. 21to FIG. 25.

While groove bottom offset 65 and groove top offset 66 are used in theembodiment shown in FIG. 10, these are changed in this secondalternative version of the second embodiment to descending rectilineargroove part 83 and ascending rectilinear groove part 84. There is anabrupt rectilinear drop from the peak to the trough of the sinusoidallywobbled groove in the descending rectilinear groove part 83. That is,the groove is formed at the peak level for ¼ wobble cycle from thegroove peak, the level then drops abruptly to the trough level, and thegroove is then formed at the trough level for the next approximately ¼wobble cycle, connecting to the groove trough. In ascending rectilineargroove part 84 there is an abrupt rectilinear rise from the trough tothe peak of the sinusoidally wobbled groove. That is, the groove isformed at the trough level through the ¼ wobble cycle from the groovetrough, the level then rises abruptly to the peak level, and the grooveis then formed at the peak level in the next approximately ¼ wobblecycle, connecting to the groove peak. These rectilinear descending andascending groove parts are referred to herein as the rectilinear grooveparts. Furthermore, a wobble wave containing a rectilinear groove part,groove phase inversion, or groove offset part is referred to as amodified wobble wave.

As shown in FIG. 22, a synchronization mark S is expressed by acombination 85 of descending rectilinear groove part 83 and ascendingrectilinear groove part 84, a negative mark (0) is recorded using onlydescending rectilinear groove part 83, and a positive mark (1) isrecorded using only ascending rectilinear groove part 84. FIG. 21 showsa descending rectilinear groove part 83 in detail.

These marks can be read using an address reader as shown in FIG. 11.

FIG. 23 shows the difference signal for rectilinear groove partscorresponding to the three marks shown in FIG. 22. These differencesignals are output by the subtracter 4 shown in FIG. 11. As will beknown from difference signal Sa(S), a difference signal that dropsabruptly to the right is obtained where there is a steeper changeoutwardly from top-to-bottom in the rectilinear groove part and adifference signal that rises abruptly to the right is obtained wherethere is a steeper change inwardly from bottom-to-top in the rectilineargroove part.

FIG. 24 shows the difference signal after it passes high pass filter 6.A difference signal that drops abruptly to the right appears as anegative pulse, and a difference signal that rises abruptly to the rightappears as a positive pulse.

FIG. 25 shows signal Si as the digitized version of the positive pulseoutput by comparator 52, and signal Sj as the digitized version of thenegative pulse output by comparator 54.

Discriminator 56 operates as follows in this case.

If either pulse signal Si or Sj is received and the other pulse signal(Si or Sj) is then also received within a first specified time (withinthe wobble period), synchronization mark S is detected and signal Sindicating the synchronization mark S is therefore output. Thissynchronization signal S is held until the next mark is detected.

If pulse signal Sj is not received within a specified time (within thewobble period) after pulse signal Si is received, positive mark (1) isdetected and a “1” signal is output indicating the positive mark (1).This “1” signal is held until the next mark is detected.

If pulse signal Si is not received within a specified time (within thewobble period) after pulse signal Sj is received, negative mark (0) isdetected and a “0” signal is output indicating the negative mark (0).This “0” signal is held until the next mark is detected.

The demodulator 14 thereafter operates as described above.

In addition to indicating whether there is a rectilinear part in thewobble groove, the descending rectilinear groove part 83 and ascendingrectilinear groove part 84 contain information indicating the direction.Separate signals Si and Sj can therefore be generated.

The descending rectilinear groove part 83 and ascending rectilineargroove part 84 can also be used to identify three different meanings (S,0, 1) in a wobble period.

Crosstalk between adjacent tracks also does not occur because thesynchronization marks, positive marks, and negative marks are within thewidth of the maximum amplitude part of the wobble.

Full CLV control is also possible because the sectors are configuredwithout changing the sector length from the inside circumference to theoutside circumference of the optical disc and it is not necessary toalign the sector block borders in the radial direction of the disc.

The grooves, synchronization marks, positive marks, and negative markscan also be cut using a single laser beam.

Furthermore, because the rectilinear part is formed across the peakamplitude part of the wobble, the position of the synchronization mark,positive mark, or negative mark can be highly precisely detected.

Yet further, because the zero cross point of the sinusoidal wobble waveand the zero cross point of the rectilinear part are the same, the clocksignal will not be disrupted at a mark when the clock signal isextracted from the wobble.

It should be noted that in this second embodiment the location of thegroove modification differs in S, 0, and 1 marks, and the location whererecording can start therefore also differs. An additional mark is neededin order to unify the positions from which recording can start. Forexample, a groove discontinuity 68 can be added as shown in FIG. 26 tothe embodiment shown in FIG. 10. More specifically, the recording startpositions can be unified by starting recording after detecting a groovediscontinuity 68.

Third Alternative Embodiment

A third alternative version of the groove modifications in the secondembodiment of the invention is described below with reference to FIG. 27to FIG. 31.

The embodiment shown in FIG. 22 uses one modified wobble wave to recordone mark. More specifically, one descending rectilinear groove part 83denotes one negative mark (0), one ascending rectilinear groove part 84denotes one positive mark (1), and one rectilinear pair 85 (containingone descending rectilinear groove part 83 and one ascending rectilineargroove part 84) denotes a synchronization mark S.

In the third alternative embodiment shown in FIG. 27, however, asuccession of modified wobble waves are used. That is, a specific pluralnumber of wobble wave cycles (such as 32 cycles) is included in theheader 102 of one sector 104 included in the sector block 105 shown inFIG. 2. To record a synchronization mark, the rectilinear pair 85 isrepeated to occupy plural cycles (such as 32 cycles in the header 102 asshown in the top row in FIG. 27. To record a negative mark (0), thedescending rectilinear groove part 83 is repeated plural times in pluralwobble wave cycles (e.g., 32 cycles) in the header 102 as shown in themiddle row in FIG. 27. To record a positive mark (1), the ascendingrectilinear groove part 84 is repeated plural times in plural wobblewave cycles (e.g., 32 cycles) in the header 102 as shown in the bottomrow in FIG. 27.

In yet another embodiment the modified wobble wave is recorded not justin the header 102 but throughout all sectors 104 containing a recordingarea 103. For example, if there are 153 wobble wave cycles in onesector, the modified wobble wave is recorded to all 153 cycles of thewobble wave.

More specifically, a modified wobble wave containing the rectilinearpair 85 is recorded for 153 continuous cycles throughout the firstsector in the sector block 105, and each rectilinear pair 85 is used torepresent synchronization data S. If a negative value 0 is to berecorded to the remaining sectors following the first sector in theblock, a modified wobble wave containing the descending rectilineargroove part 83 is recorded for 153 continuous cycles throughout eachsector. Likewise, if a positive value 1 is to be recorded to theremaining sectors, a modified wobble wave containing the ascendingrectilinear groove part 84 is recorded for 153 continuous cyclesthroughout the sector.

It will be apparent that it is not necessary to repeat the modifiedwobble wave throughout the sector, and it can be repeated a certainplural number of cycles at any part of the sector. Furthermore, theplural cycles in which the modified wobble wave is recorded can benon-contiguous, such as every other cycle. By thus inserting spacebetween the cycles containing the modified wobble wave other informationcan also be recorded by measuring the gap between the cycles.

By thus recording data to the wobble waves using modified wobble wavesas described above it is not necessary to use track space to record thesynchronization mark S, positive mark (1), or negative mark (0), anddata can be extracted by observing the shape of the modified wobblewaves of the track. It is therefore not necessary to insert thesynchronization mark S, positive mark (1), or negative mark (0) to theheader 102 or other specific location, and they can be recorded at adesirably location.

A discontinuity 86 is also recorded in the first wobble wave as shown inthe top row in FIG. 27 in order to make detecting the start of thesector block easier and more reliable. This discontinuity 86 can bedisposed to the peak of the wobble wave as shown in FIG. 27 or in thetrough (that is, at a peak amplitude part of the wave), or at the zerocross point of the descending rectilinear groove part 83 or ascendingrectilinear groove part 84 (that is, at the minimum amplitude part ofthe wave). The discontinuity 86 is preferably disposed at the zero crosspoint because the discontinuity 86 will then not produce unnecessarynoise during wobble wave frequency detection. It will be further notedthat this location of discontinuities also applies to thediscontinuities described in the first embodiment above.

It will be noted that the discontinuity 86 in FIG. 27 is formed byinterrupting the track groove and overwriting data to the discontinuity86 is therefore difficult. This is because light reflection differsgreatly depending on whether or not the groove is present and thediscontinuity 86 behaves like noise in the playback signal. In thepresent embodiment, therefore, the area containing such a discontinuity86 (such as block 85) is used as a VFO recording area. A VFO recordingarea is an area-where a monotone VFO signal is recorded for generatingthe PLL used to playback the data recorded after the VFO recording area.Some variation in such external noise simply appears as local jitter ina VFO area, and will not directly produce an error. Furthermore,frequency separation of noise caused by the discontinuity 86 is alsopossible because the VFO signal is a monotone signal.

FIG. 31 is a block diagram of a reader for reading a modified wobblewave as shown in FIG. 27.

The reader shown in FIG. 31 comprises a rectilinear wave detector 90,discontinuity detector 91, and distribution detector 92. The rectilinearwave detector 90 uses the major parts of the address reader shown inFIG. 11. Waveforms of the signals at major points in the rectilinearwave detector 90 are shown in FIG. 28, FIG. 29, and FIG. 30.

FIG. 28 shows the difference signals for the three modified wobble wavesshown in FIG. 27. These difference signals are output by the subtracter4 shown in FIG. 31. This subtracter 4 operates as described withreference to FIG. 11.

FIG. 29 shows the difference signals after passing the high pass filter6. A difference signal that drops abruptly to the right appears as anegative pulse, and a difference signal that rises abruptly to the rightappears as a positive pulse.

FIG. 30 shows signal Si as the digital version of the positive pulseoutput by comparator 52, and signal Sj as the digital version of thenegative pulse output by comparator 54. In a modified wobble wavecontaining repeated rectilinear pairs 85, a pulse appears in bothsignals Si and Sj. These pulses appear once per cycle in the modifiedwobble wave.

Operation when the modified wobble wave has 153 cycles per sector isdescribed next. In the first sector (the sector containing thesynchronization mark S) there are 153 pulses in signal Si and 153 pulsesin signal Sj. If the following sector records 0 data (negative mark (0))there are no pulses in signal Si and 153 pulses in signal Sj. If thefollowing sector records 1 data (positive mark (1)) there are 153 pulsesin signal Si and no pulses in signal Sj. Note that due to noise andother factors the actual number of pulses may vary.

The discontinuity detector 91 shown in FIG. 31 uses the major parts ofthe address reader shown in FIG. 4. As described with reference to FIG.5, a pulse is output when a discontinuity 86 is detected. Note that thesubtracter 4 disposed in discontinuity detector 91 can be changed to anadder. When a subtracter is used the discontinuity 86 can only bedetected when it is near a wobble wave peak, but when an adder is useddiscontinuity 86 can be detected near the peak and near the zero cross.

The distribution detector 92 shown in FIG. 31 is described next.

The distribution detector 92 comprises pulse counters 93 and 94,comparators 95, 96, 97, sector synchronization counter 98, and latch 99.Pulse counters 93 and 94 count the number of pulses in signals Si andSj, respectively. Pulse counter 93 outputs the accumulated count toinput b of comparators 95, 96, 97. If a>b (where a is the count appliedto input a, and b is the count applied to input b) and the difference ispreferably sufficiently great (that is, a>>b), comparator 95 outputshigh. If a<b and the difference is preferably sufficiently great (thatis, a<<b), comparator 96 outputs high. If a≈b and the difference ispreferably sufficiently small, comparator 97 outputs high.

These high signals are applied to the latch 99. If a high signal isreceived from comparator 95, latch 99 outputs a 1 indicating a positivemark (1). This 1 signal is held until data for the next sector isdetected. If the latch 99 receives a high from comparator 96, latch 99outputs a 0 signal indicating a negative mark (0). This 0 signal is helduntil data for the next sector is detected. If a high from comparator 97is detected, latch 99 outputs an S signal indicating a synchronizationmark S. This S signal is held until data for the next sector isdetected.

The sector synchronization counter 98 counts the number of cycles in thesynchronization signal (the same number of cycles as the wobble wave,but the wobble wave contains noise and the number is not stable). Thesynchronization signal is generated by a PLL circuit from the detectedwobble signal, for example. First, the count is reset to zero at thediscontinuity detection pulse from the discontinuity detector 91. Thenumber of pulses in the synchronization signal, that is, thesynchronization pulses, is then counted. The wobble wave has 153 cyclesper sector in the present embodiment as rioted above. A reset signal istherefore output to the pulse counters 93 and 94 and latch 99 every time153 pulses are counted, and the pulse counters 93 and 94 are reset.

The distribution detector 92 compares the number of pulses in signal Siin one sector with the number of pulses in signal Sj. If the number ofsignal Si pulses is sufficiently greater than the number of signal Sjpulses, comparator 95 outputs high. Conversely, if the number of signalSj pulses is sufficiently greater than the number of signal Si pulses,comparator 96 outputs high. If the number of Si pulses and Sj pulses isalmost equal, comparator 97 outputs high. The latch 99 latches a highsignal from any of comparators 95, 96, 97 and appropriately outputs a 1or 0 signal. The sector synchronization counter 98 is reset by an Ssignal.

Subsequent signal processing is handled by the demodulator 14 asdescribed above.

The 1, 0, and S signals can be detected more accurately by thusrepeating the modified wobble wave. Furthermore, adverse effects of thewobble wave on the synchronization signal that must be detected can beminimized if a modified wobble wave containing a rectilinear componentas described above is included in the modified wobble wave.

Fourth Alternative Embodiment

FIG. 32 shows the major components of a fourth alternative embodiment.In the embodiment shown in FIG. 32 the length of the positive amplitudeparts and negative amplitude parts of the wobble wave differ so that theduty ratio can be changed without changing the wobble frequency. Morespecifically, in FIG. 32 the length of the negative amplitude part 180of the wobble wave is longer than the positive amplitude part, and thelength of the positive amplitude part 181 is longer than the negativeamplitude part. The wobble is thus formed so that this part 180 islonger in a negative mark (0) and part 181 is longer in a positive mark(1) as shown in FIG. 32. It is therefore not necessary to differentiatethe playback signal when discriminating the negative and positive datamarks and the effects of noise can be reduced because a clock timer, forexample, can be used to measure the duty ratio.

Fifth Alternative Embodiment

FIG. 33 shows the major components of a fifth alternative embodiment.While a discontinuity 86 is formed in the first wobble wave in theembodiment shown in FIG. 27, a mark 212 locally increasing the trackgroove width is formed in this embodiment shown in FIG. 33.

This mark 212 is used to detect the beginning of a sector block and isreferred to as a block mark. The configuration shown in FIG. 33 does notproduce a discontinuity interrupting the groove, and information otherthan the VFO signal can therefore be recorded using block marks. As aresult, overhead can be reduced.

Sixth Alternative Embodiment

FIG. 34 shows the major components of a sixth alternative embodiment.The variation shown in FIG. 34 forms a block mark 213 creating a localincrease in groove wobble amplitude. Similarly to the variation shown inFIG. 33, this embodiment does not cause a discontinuity in the groove,and information other than the VFO signal can therefore be recordedusing block marks.

Seventh Alternative Embodiment

FIG. 35 shows the major components of a seventh alternative embodiment.In this variation a wobble is formed only to one edge of the trackgroove. The preceding embodiments and variations apply particularly toso-called groove-recording optical discs that record data to the trackgroove, but there are also so-called land and groove optical discs thatrecord data to both grooves and lands (the space between grooves) alongthe track. This seventh alternative embodiment of the invention appliesto such land and groove type optical discs.

In the disc shown in FIG. 35 either negative data (0) (indicated by area221) or positive data (1) (indicated by area 231) is recorded along oneedge of the groove. This enables both the groove 2 and adjacent land 4to be addressed by the same address. Data is recorded to both the land 4and groove 2. This configuration enables the track pitch to be furtherreduced so that recording density can be further increased.

As will be known from the preceding description, the present inventionforms a wobble of a specific shape and cycle in a unit period of thetrack groove and records different shapes differing according touniformly defined secondary information in said unit period. The presentinvention can therefore provide an optical disc medium that is suitableto high density recording, can record address information that reducesor eliminates overhead, and can generate a monotone wobble playbacksignal.

1. An information media comprising: a track; and a wobbled groove formedalong said track; wherein said wobbled groove contains positive marksand negative marks, and wherein at least one of said positive marks isused for indicating one of logical “0” and “1” and at least one of saidnegative marks is used for indicating the other one of logical “0” andor “1”, respectively.
 2. An information media according to claim 1,wherein a wobble of said wobbled groove, compared to a sinusoidalwobble, contains a steeper outwardly inclination at positive marks, anda steeper inwardly inclination at negative marks.
 3. An informationmedia according to claim 2, wherein one of logical “0” and “1” isindicated by a plurality of said positive marks, and the other one of alogical “0” and “1” is indicated by a plurality of said negative marks,respectively.
 4. An information media according to claim 1, wherein oneof logical “0” and “1” is indicated by a plurality of said positivemarks, and the other one of a logical “0” and “1” is indicated by aplurality of said negative marks, respectively.
 5. An information mediaaccording to claim 1, wherein said wobbled groove contains a combinationof said positive marks and said negative marks for indicating an addresssignal.
 6. An information media according to claim 1, wherein saidwobbled groove contains a combination of at least one of said positivemarks and at least one of said negative marks for indicating asynchronization signal.
 7. A reproducing apparatus for reproducing aninformation signal from an information media having a wobbled grooveformed along a track, wherein the wobbled groove contains positive marksand negative marks, and wherein at least one of the positive marks isused for indicating one of logical “0” and “1” and at least one of thenegative marks is used for indicating the other one of logical “0” and“1”, respectively, said reproducing apparatus comprising: a pickup unitoperable to read the information signal recorded on the informationmedia; a detector operable to detect at least one of the positive marksand at least one of the negative marks from the read signal, and outputat least one positive mark signal and at least one negative mark signal;a generator operable to generate 1s and 0s according to the at least onepositive mark signal and the at least one negative mark signal; and aconverter operable to convert the 1s and 0s produced from said generatorto an address signal.
 8. A reproducing apparatus according to claim 7,wherein a logical “1” is represented by at least one of the positivemarks and a logical “0” is represented by at least one of the negativemarks.
 9. A reproducing apparatus according to claim 8, wherein saiddetector comprises a high pass filter operable to output a signal, and acomparator operable to compare the signal output from said high passfilter with a predetermined level.
 10. A reproducing apparatus accordingto claim 8, wherein said generator generates 1s and 0s according to aplurality of the positive mark signals and a plurality of the negativemark signals.
 11. A reproducing apparatus according to claim 10, whereinsaid detector comprises a high pass filter operable to output a signal,and a comparator operable to compare the signal output from said highpass filter with a predetermined level.
 12. A reproducing apparatusaccording to claim 7, wherein said generator generates 1s and 0saccording to a plurality of the positive mark signals and a plurality ofthe negative mark signals.
 13. A reproducing apparatus according toclaim 12, wherein said detector comprises a high pass filter operable tooutput a signal, and a comparator operable to compare the signal outputfrom said high pass filter with a predetermined level.
 14. A reproducingapparatus according to claim 7, wherein said detector comprises a highpass filter operable to output a signal, and a comparator operable tocompare the signal output from said high pass filter with apredetermined level.